Identification of hydrological model parameters variation using ...

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Jan 26, 2016 - and Guo, 2012; Li et al., 2013; Zhang et al., 2013; Xiong et al., 2014). The inputs of the model include. 81 monthly areal precipitation and ...
Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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Identification of hydrological model parameters variation using

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ensemble Kalman filter

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Chao Deng1,2, Pan Liu1,2,*, Shenglian Guo1,2, Zejun Li1,2, Dingbao Wang3

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Wuhan, China

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Hubei Provincial Collaborative Innovation Center for Water Resources Security, Wuhan, China

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Department of Civil, Environmental & Construction Engineering, University of Central Florida,

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State Key Laboratory of Water Resources and Hydropower Engineering Science, Wuhan University,

Orlando, USA

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*Corresponding author: P. Liu, State Key Laboratory of Water Resources and Hydropower

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Engineering Science, Wuhan University, Wuhan 430072, China

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Email: [email protected]

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Tel: +86-27-68775788; Fax: +86-27-68773568

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Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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Abstract: Hydrological model parameters play an important role in the ability of model prediction. In

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a stationary content, parameters of hydrological models are treated as constants. However, model

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parameters may vary dynamically with time under climate change and human activities. The technique

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of ensemble Kalman filter (EnKF) is proposed to identify the temporal variation of parameters for a

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two-parameter monthly water balance model by assimilating the runoff observations, where one of state

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equations is that the model parameters should not change much within a short time period. Through a

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synthetic experiment, the proposed method is evaluated with various types of parameter variations

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including trend, abrupt change, and periodicity. The application of the method to the Wudinghe basin

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shows that the water storage capacity, a parameter in the model, has an apparent increasing trend during

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the period from 1958 to 2000. The identified temporal variation of water storage capacity is explained

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by land use and land cover changes due to soil and water conservation measurements. Whereas, the

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application to the Tongtianhe basin demonstrates that the parameter of water storage capacity has no

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significant variation during the simulation of 1982-2013, corresponding to the relatively stationary

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catchment characteristics. Additionally, the proposed method improves the performance of hydrological

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modeling, and provides an effective tool for quantifying temporal variation of model parameters.

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Keywords: model parameter identification, temporal variation of parameter, catchment characteristics,

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ensemble Kalman filter 2

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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1 Introduction

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Hydrological model parameters are critically important for accurate simulation of streamflow. In

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hydrological modeling, parameters are usually assumed to be stationary, i.e., the calibrated parameters

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are a set of constants during the calibration period, and have extrapolative ability outside the range of

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the observations used for parameter estimation (Merz et al., 2011). However, the calibration period may

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contain different climactic condition and hydrological regime, and has a significant impact on the model

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parameter estimation (Merz et al., 2011; Zhang et al., 2011; Westra et al., 2014; Patil and Stieglitz,

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2015). The model parameters may potentially change responding to time-variable precipitation and

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other inputs. For example, land use and land cover changes contribute to temporal change of model

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parameters (Andréassian et al., 2003; Brown et al., 2005; Merz et al., 2011). Consequently, assuming

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time invariant model parameters may be unrealistic, especially for catchments with time-varying

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climate conditions and/or catchment properties.

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The situation of time-variant hydrological model parameters has been reported in a few publications

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(Merz et al., 2011; Brigode et al., 2013; Westra et al., 2014; Patil and Stieglitz, 2015). For example, Ye

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et al. (1997) and Paik et al. (2005) mentioned the seasonal variations of hydrological model parameters.

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Merz et al. (2011) analyzed the temporal changes of model parameters which were calibrated

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respectively by using six consecutive 5 year periods between 1976 and 2006 for 273 catchments in 3

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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Austria. Recently, Westra et al. (2014) proposed a strategy to cope with nonstationary of hydrological

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model parameters, which were represented as a function of a set of time-varying covariates before using

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an optimization algorithm for calibration. Previous studies provided two main methods to identify the

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time-variant model parameters: (1) Divide the historical record into consecutive subsets, and then

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calibrate the model parameters using an optimization algorithm (e.g., Merz et al. (2011)). The model

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parameters are fixed values in each subset. (2) Build the functional form of the selected time-variant

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model parameters, and calibrate the model parameters using an optimization algorithm based on the

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entire historical record (e.g., Westra et al. (2014)).

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The data assimilation (DA) method has been used to estimate both model parameters and state variables.

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For example, Vrugt et al. (2013) proposed two types of Particle-DREAM method to track the evolving

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target distribution of model parameters. Although the DA method has been used to estimate model

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parameters, the objective is to identify the fixed values of parameters. Additionally, little attention has

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been paid to the identification of time-variant model parameters and the interpretation of their temporal

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variations based on the climate conditions and/or catchment characteristics.

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The aim of this study is to assess the capability of the DA method (i.e., the EnKF) to identify the

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temporal variation of parameters for a monthly water balance model, and to link the parameter 4

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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variations to changes in physical properties.

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The remainder of this paper is organized as follows. Section 2 presents a brief review of the

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two-parameter monthly water balance model and the EnKF method. Following the methodology,

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Section 3 describes the synthetic experiment and the application to two case studies. Results and

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discussion are presented in Section 4, followed by conclusions in Section 5.

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2 Methodology

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2.1 Monthly water balance model

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The two-parameter monthly water balance model, developed by Xiong and Guo (1999), has been

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widely applied for monthly runoff simulation and forecast (Guo et al., 2002; Guo et al., 2005; Xiong

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and Guo, 2012; Li et al., 2013; Zhang et al., 2013; Xiong et al., 2014). The inputs of the model include

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monthly areal precipitation and potential evapotranspiration. The actual monthly evapotranspiration is

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calculated as follows:

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Ei  C  EPi  tanh  Pi / EPi 

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where Ei represents the actual monthly evapotranspiration; EPi and Pi are the monthly potential

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evapotranspiration and precipitation, respectively; C is the first model parameter; and i is the time

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step.

(1)

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Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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The monthly runoff is dependent on the soil water content and is calculated by the following formula:

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Qi  Si  tanh  Si / SC 

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where Qi is the monthly runoff; and Si is the soil water content. As the second model parameter,

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SC represents the water storage capacity of the catchment with the unit of millimeter. The available

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water for runoff at the i th month is computed by Si 1  Pi  Ei . Then, the monthly runoff is calculated

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by:

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Qi   Si 1  Pi  Ei   tanh  Si 1  Pi  Ei  / SC 

(2)

(3)

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Finally, the soil water content at the end of each time step is updated based on the water conservation

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law:

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Si  Si 1  Pi  Ei  Qi

(4)

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2.2 Ensemble Kalman filter

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EnKF is a sequential data assimilation technique based on the Monte Carlo method and produces an

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ensemble of state simulations to update the state variables and model parameters, conditioned on a

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series of model observations (Moradkhani et al., 2005; Shi et al., 2014). It has been successfully

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applied into dozens of hydrological applications (Abaza et al., 2014; DeChant and Moradkhani, 2014; 6

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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Delijani et al., 2014; Samuel et al., 2014; Tamura et al., 2014; Xue and Zhang, 2014; Deng et al.,

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2015). In EnKF, the state equation is as follows:

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i 1  i   i ,  i ~ N  0, Ri 

(5)

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xi 1  f  xi ,i 1    i ,  i ~ N  0, Gi 

(6)

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where xi is the state vector with a dimension of n  1 at time i ; i1 is the parameter vector with a

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dimension of l  1 at time i  1 ; f is the forward operator;  i and  i are the independent white

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noise for the forecast model with a dimension of n  1 , followed a Gaussian distribution with zero

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mean and covariance matrix Gi and Ri with a dimension of n  n , respectively. Equation (5)

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indicates that hydrological parameters should not change much within a short time period.

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The observation equation is as follows:

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yi 1  h  xi 1 , i 1   i 1 , i 1 ~ N  0, Si 1 

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where yi 1 is the observation vector with a dimension of m  1 at time i  1 ; h is the

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observational operator which represents the relationship between the observations and states; i 1 is

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the noise term with a dimension of m  1 which follows a Gaussian distribution with zero mean and

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covariance matrix Si 1 with a dimension of m  m .

(7)

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Based on the available state and observation equations, the EnKF assimilation process can be 7

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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expressed as follows:

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(1) Set the ensemble size N and the total length of the historical record n .

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(2) Generate the ensemble of model parameters and state variables by perturbing the updated values

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from the previous time step.

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ik1 i  iki   ik

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xik1 i  f xiki ,ik1 i   ik

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where ik1 i is the kth ensemble member forecast at time i  1 ; iki is the kth updated ensemble

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member at time i ;  i is the white noise for the kth ensemble member; xik1 i is the kth ensemble

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member forecast at time i  1 ; xiki is the kth updated ensemble member at time i ; and  ik is the

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white noise for the kth ensemble member.

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(3) Generate the ensemble of runoff observations by adding a perturbation:

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yik1  yi 1  ik1

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where yik1 is the kth observation ensemble member at time i  1 ; and ik1 is the observation error

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for the kth ensemble member.



(8)



(9)

(10)

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The model parameters and state variables are updated according to the following equations:

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xik1 i 1=xik1 i  Kix1 yik1  h xik1 i ,ik1 i

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ik1 i 1=ik1 i  Ki1

 y

k i 1

  hx

k i 1 i

,ik1 i

 

(11) (12) 8

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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Note that the parameter and state vectors are updated following the approach in the previous studies

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(Wang et al., 2009; Nie et al., 2011; DeChant and Moradkhani, 2012; Lü et al., 2013). Ki 1 is the

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Kalman gain matrix that represents the weight between the forecasts and observations. It can be

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calculated by (Moradkhani et al., 2005):

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K ix1  ixy1 i iyy1 i  Si 1

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K i1  i y1 i

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 ixy1 i =

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 

yy i 1 i

 Si 1

 

1

(13)

1

(14)

1 X YT N  1 i 1 i i 1 i 1 i y1 i =  YT N  1 i 1 i i 1 i 1  iyy1 i = Yi 1 iYi T1 i N 1

(15) (16) (17) y

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where i 1 i is the cross covariance of the forecasted states; i 1 i is the cross covariance of the forecasted

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parameters; i 1 i is the error covariance of the forecasted output; X i 1 i = xi 1 i  xi 1 i ,  , xi 1 i  xi 1 i

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is the ensemble mean of the forecasted states; i 1 i =

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of the forecasted parameters; Yi 1 i = yi 1 i  yi 1 i ,  , yi 1 i  yi 1 i

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forecasted output; N is the number of ensemble members; and the superscript T represents the matrix transpose.

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Since the parameters are limited within an interval, the constrained EnKF is used (Wang et al., 2009) in this study.

xy



yy



1



1 i 1 i

m

1

m

 im1 i ,  , iN1 i  im1 i N

m





and

N

m



m

and xi 1 i

im1 i is the ensemble mean

m

and yi 1 i is the ensemble mean of the

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The ensemble size, uncertainties in input and output have significant impacts on the assimilation 9

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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performance of the EnKF, and they are determined based on previous studies (Wang et al., 2009; Xie

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and Zhang, 2010; Lü et al., 2013; Samuel et al., 2014). The ensemble size is set to 1000 for all cases.

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In the present study, the uncertainties including parameter errors (  , Eq. (8)), state variable error (  ,

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Eq. (9)) and streamflow observation error (  , Eq. (10)), are assumed to follow a Gaussian distribution.

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In terms of the parameter errors, the standard deviation for C is set to 0.01 for all the cases, while

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that of SC are set from 0.5 to 5 to account for its uncertainties. The standard deviation of both model

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state and observation errors are assumed to be proportional to the magnitude of true values, and the

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scale factors are set to be 5% and 10% respectively for all cases (Wang et al., 2009; Lü et al., 2013). It

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should be noted that the variable variance multiplier can be used to perturb the observations

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(Leisenring and Moradkhani, 2012; Yan et al., 2015).

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2.3 Evaluation index

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Two evaluation criteria, including the Nash-Sutcliffe efficiency (NSE) (Nash and Sutcliffe, 1970) and

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the volume error (VE) are used to evaluate the runoff assimilation results for the synthetic experiment

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and application to catchments (Deng et al., 2015; Li et al., 2015).

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 Q NSE  1   Q n

 Qobs ,i 

i 1

sim ,i

n

obs ,i  Q obs

i 1



2

(18)

2

10

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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 VE 

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where Qsim ,i and Qobs ,i are the simulated and observed runoff for the i th month; Q sim and Q obs

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are the mean of the simulated and observed runoff, respectively for the i th month; and n is the total

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number of data points. The NSE has been widely used to assess the goodness-of-fit for hydrological

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modeling. A NSE value of 1 means a perfect match of simulated runoff to the observations. The VE is

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a measure of bias between the simulated and observed runoff. For example, VE with the value of 0

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denotes no bias, and a negative value means an underestimation of the total runoff volume.

n i 1

Qsim,i   i 1 Qobs ,i n

(19)

 i1 Qobs,i n

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3 Data and study area

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3.1 Synthetic experiment

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A synthetic experiment is designed to evaluate the capability of the assimilation procedure to identify

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the temporal variation of model parameters. The model parameters are given with specific variation

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including trend, abrupt change and periodicity. Observations for precipitation and potential

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evapotranspiration are generated via a stochastic simulation, and runoff is then produced by using the

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monthly water balance model. The steps toward identifying temporal variation of model parameters are

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as follows:

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(1) Scenarios set: Generate the time-variant parameters with different trend variations, potential

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evapotranspiration and precipitation on a monthly time scale, then compute the runoff observations 11

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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using the two-parameter monthly water balance model.

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(2) Initialization: Specify the ensemble size and the total number of assimilation time steps. At the first

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time step, the model parameter and state variable ensembles are generated using a predefined Gaussian

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distribution based on the prior intervals in Table 1.

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(3) Data assimilation: After the initialization of parameters and state variables, the hydrologic model

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parameters and state are updated by assimilating the runoff observations obtained in Step (1). Note that

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the model parameters and state, as well as the runoff observations, are perturbed with an error item

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which is assumed a Gaussian distribution with zero mean and specified variance.

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The data set used in this experiment has a total length of 672 months. The first 24 months is set as

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model warm-up period to reduce the impact of the initial hydrological conditions. The experiment is

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implemented to identify the variation of model parameters from the scenarios in Table 2, respectively.

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The assimilated parameter results are evaluated using the following criteria, including the Pearson

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correlation coefficient (R), the root mean square error (RMSE) and mean absolute relative error

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(MARE):

 x  x n

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R

i 1

n

i 1

sim ,i

 xsim  xobs ,i  xobs 

sim ,i  xsim   xobs ,i  xobs  2

(20)

2

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Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

2 1 n xsim,i  xobs ,i    i 1 n

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RMSE 

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MARE 

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where xsim ,i and xobs ,i are the assimilated and observed model parameters for the i th month; x sim

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and x obs are the mean of the assimilated and observed model parameters, respectively for the i th

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month; n is the total number of data points.

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3.2 Study area

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3.2.1 Case 1: Wudinghe basin

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The method is applied in the Wudinghe basin (Fig. 1) located in the southern fringe of Maowusu

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Desert and the northern part of the Loess Plateau in China with a semiarid climate. It has a drainage

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area of approximately 30,261 km2 and a total length of 491 km and forms a part of the Yellow River

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basin. The Wudinghe basin has an average slope of 0.2%, and its elevation ranges from 600 to 1800 m

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above the sea level. The Baijiachuan gauge station, which is the most downstream station of the

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Wudinghe basin, drains 98% of the total catchment area. The mean annual precipitation over the basin

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is 401 mm, of which 72.5% occurs in the rainy season from June to September (Fig. 2). The mean

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annual potential evapotranspiration is 1077 mm, and the mean annual runoff is about 39 mm with a

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runoff coefficient of 0.1.

(21)

1 n xsim ,i  xobs ,i  n i 1 xobs ,i

(22)

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Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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3.2.2 Case 2: Tongtianhe basin

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The Tongtianhe basin (Fig. 3) is located in southwestern Qinghai Province in China with a continental

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climate. It belongs to the source area of Yangtze River basin with a drainage area of about 140,000 km2

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and a total main stream length of 1206 km. The elevation of the Tongtianhe basin approximately ranges

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from 3500 to 6500 m above the sea level. Zhimenda is the basin outlet. The mean annual precipitation

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over the basin is 440 mm, of which 76.9% occurs in the period from June to September (Fig. 4). The

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mean annual potential evapotranspiration is 796 mm, and the mean annual runoff is about 99 mm with a

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runoff coefficient of 0.23. The Tongtianhe basin is barely affected by human activities owing to the

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limitation of the topographic condition and the water conservation measures conducted by the

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government. It should be noted that the Tongtianhe basin is used for comparative study on model

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parameter identification, where has no significant impacts from the climate change and human

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activities.

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3.2.3 Data

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The data set including monthly precipitation, potential evapotranspiration and runoff in Wudinghe basin

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(from 1956 to 2000) and Tongtianhe basin (from 1980 to 2013) are used in this study. The potential

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evapotranspiration is estimated using the Penman-Monteith equation (Allen et al., 1998) based on the

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meteorological data from the China Meteorological Data Sharing Service System (http://cdc.nmic.cn). 14

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

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To reduce the impact of the model initial conditions, a 2-year data set, i.e., from 1956 to 1957 for

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Wudinghe basin and from 1980 to 1981 for Tongtianhe basin, is reserved as the warm-up period. The

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runoff estimations from the SCE-UA method (Duan et al., 1993) are compared with that of the EnKF.

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4 Results and discussion

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4.1 Synthetic experiment

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To assess the performance of the EnKF, the assimilated results are examined for the four scenarios in

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the synthetic experiment. The comparisons of the assimilated and true model parameters under

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different scenarios are presented from Fig. 5 to Fig. 8, and Table 3 shows the evaluation statistics for

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both the parameters and runoff assimilations. All these four figures show that the assimilated

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parameters of C and SC have similar trends as the true ones. These figures demonstrate that the

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SC assimilation performs better than the C assimilation. The runoff assimilation results (see Table

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3, penultimate and last columns) show that the estimation of runoff using the EnKF perfectly matches

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the observations with NSEs of 0.99 and VEs of approximately zero. It should be noted that there is a

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time lag in assimilated C for the periodic case. In EnKF, the observation at the current time is used

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to adjust the state variables and parameters, and the updates of parameters depend on the Kalman gain

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for parameters.

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The above results demonstrate that the EnKF is able to identify the temporal variation of the model

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parameters by updating the state variable and parameters based on the runoff observations. The

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estimated parameters for the cases of trend or abrupt change match the true values better than the case

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with periodic variation.

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4.2 Case studies

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Fig. 9 illustrates the double mass curve of monthly runoff and precipitation for Wudinghe and

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Tongtianhe basins, respectively. The top panel shows the linear relationship between cumulative runoff

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and precipitation before and after the turning point of January 1972 in the Wudinghe basin, which is

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same as the result presented by Li et al. (2014). The results show two straight lines with different slopes

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for the relationships between precipitation and runoff, indicating that changes occurred. While the

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bottom panel demonstrates a single linear relationship fits all the data for the Tongtianhe basin,

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suggesting a stable precipitation-runoff relationship during the 1982-2013 period.

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The temporal variation of estimated SC and the associated 95% uncertainty interval are shown in Fig.

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10. The top panel shows an apparent increasing trend with two stages in Wudinghe basin. The first stage

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is from January 1958 to December 1971, when the water storage capacity has a significant increasing

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trend with a slope of 0.059. The water storage capacity in the second stage, from January 1972 to 16

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

282

December 2000, has an obvious increasing trend with a slope of 0.022. The temporal variation of water

283

storage capacity is related to the change of catchment properties, such as the land use and land cover

284

change. Since the 1960s, the soil and water conservation measures, including tree and grass planting,

285

reservoir construction and land terracing, have been undertaken to cope with the soil erosion in

286

Wudinghe basin. During the 1970s, large-scale engineering measures were effectively implemented,

287

which improved the water holding capacity of the basin directly, and also provided a reasonable

288

physical explanation for the increasing trend and its degree of SC in the first stage. In the second stage,

289

the water storage capacity increases slower than the first stage since the engineering measures have

290

almost finished. Another important factor is the reduction of storage capacity for reservoirs caused by

291

sediment accumulation. In the 1980s, lots of measures were adopted for comprehensive management

292

within small catchments for further soil erosion control, which resulted in increasing grassland, forest

293

land and terracing land. These land use changes played a significant role in increasing water storage

294

capacity. On the other hand, the result of Tongtianhe basin shows that the estimated SC has no

295

pronounced trend since the R value has an insignificance level. Moreover, the range of variation in

296

estimated SC values is much smaller compared to those of the Wudinghe basin. The grey regions

297

represent the 95% uncertainty intervals obtained from the parameter ensemble. The results demonstrate

298

that the EnKF performs well for parameter estimation with narrow uncertainty bounds. Fig. 11 shows

299

the temporal variation of estimated C values and the 95% uncertainty ranges for both Wudinghe basin 17

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

300

and Tongtianhe basin. The results demonstrate that the estimated C has a stable value, with slopes that

301

are almost zero for both the cases. The narrow uncertainty bounds indicate that the EnKF can provide

302

superior performance of parameter estimation.

303 304

Fig. 12 illustrates the comparison of the observed and estimated runoff from the EnKF and SCE-UA for

305

both Wudinghe and Tongtianhe basins. The evaluation results are shown in Table 4. The NSEs from the

306

EnKF and SCE-UA in the Wudinghe basin are 0.93 and 0.16, and the VEs are 0.07 and 0, respectively.

307

While the corresponding index values from the EnKF and SCE-UA are 0.99 and 0.79, 0.04 and 0 in the

308

Tongtianhe basin. Therefore, the EnKF has superior performance compared to the SCE-UA for both

309

case studies. The results show that the data assimilation improves the runoff estimation.

310 311

In summary, these analyses show that the EnKF can identify the temporal variation of model parameters

312

well by updating both state variables and parameters based on the runoff observations. Moreover, the

313

trends of parameter SC can be explained by the change of catchment characteristics. On the contrary,

314

the estimated SC is approximately stable when the catchment is barely affected by human activities.

315

Consequently, the EnKF provides effective performance for time-variant parameter identification.

316 317

5 Conclusions 18

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

318

This study proposes an ensemble Kalman filter (EnKF) to identify the temporal variation of model

319

parameters in a monthly water balance. A synthetic experiment, which contains four scenarios of model

320

parameter variation, is designed to demonstrate the ability of the EnKF for identifying the temporal

321

variation of the model parameters using the runoff observations. The main conclusions are drawn as

322

follows.

323 324

Based on EnKF, the variation of model parameters can be effectively identified by assimilating runoff

325

observations. The EnKF can provide accurate results for parameter identification even though slight

326

time lags exist when parameters have periodic variations.

327 328

Then, the EnKF method is applied to the Wudinghe basin in China, aiming to detect the temporal

329

variability of model parameters and to provide an explanation for the parameter variation from the

330

perspective of catchment property change. Meanwhile, a comparative study is implemented to

331

investigate the variation of model parameters in Tongtianhe basin where human activities barely exist.

332

The parameter of water storage capacity ( SC ) for the monthly water balance model shows a significant

333

increasing trend for the period of 1958 to 2000 in the Wudinghe basin. The soil and water conservation

334

measures, including tree and grass planting, reservoir building and land terracing, have been

335

implemented during 1958 to 2000, resulting in the increase of the water holding capacity of the basin, 19

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

336

which explains the increasing trends of SC . Moreover, the magnitudes of the engineering measures in

337

different time periods play an important role in the degree of increasing trend for SC. In the Tongtianhe

338

basin, the parameter SC has no significant trend for the period of 1982 to 2013, which is consistent

339

with the relatively stationary catchment characteristics.

340 341

The method proposed in this paper provides an effective tool for the time-variant model parameters

342

identification. Future work will be focused on the influence of the correlations between/among model

343

parameters and performance comparison of multiple data assimilation methods.

344 345

Acknowledgments

346

This study was supported by the Excellent Young Scientist Foundation of NSFC (51422907). The

347

authors would like to thank the editor and the anonymous reviewers for their comments that helped

348

improve the quality of the paper.

349 350

References

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Tables Table 1. Description and prior ranges of the two parameters for the monthly water balance model. Parameters and state variable Parameter State variable

Description

Interval and unit

C

Evapotranspiration parameter

0.2-2.0 (-)

SC

Catchment water storage capacity

100-2000 (mm)

S

Soil water content

mm

465

24

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466 467

Table 2. Scenarios of time-variant model parameters in the synthetic experiment. Scenario

Description

Scenario 1

C has a periodic variation, and SC has an increasing trend

Scenario 2

C has a periodic variation, and SC has an abrupt change

Scenario 3

C has a periodic variation with an increasing trend, and SC has an increasing trend

Scenario 4

C has a periodic variation with an increasing trend, and SC has an abrupt change

468

25

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469 470

Table 3. Performance statistics for parameter and runoff estimations in the synthetic experiment. Scenario

Parameter

RMSE

R

MARE

Scenario 1

C SC C SC C SC C SC

0.15 182.87 0.16 156.19 0.12 180.27 0.12 156.42

0.554 0.987 0.633 0.957 0.636 0.992 0.695 0.969

0.21 0.03 0.19 0.04 0.12 0.03 0.12 0.03

Scenario 2 Scenario 3 Scenario 4

471

26

NSE (Runoff)

VE (Runoff)

0.99

0.0007

0.99

0.0001

0.99

-0.0012

0.99

-0.0009

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

472 473 474 475

Table 4. Comparison of monthly runoff simulation performance between the optimization algorithm (SCE-UA) and the data assimilation method (EnKF) in Wudinghe basin within the period 1958-2000 and Tongtianhe basin within the period 1982-2013, respectively. Area

Method

NSE

VE

Wudinghe basin

SCE-UA

0.16

0

EnKF

0.93

0.07

SCE-UA

0.79

0

EnKF

0.99

0.04

Tongtianhe basin

27

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476

Figures

477 478

Figure. 1. Location of Wudinghe basin.

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479

480 481

Figure. 2. Mean monthly precipitation and runoff from 1956 to 2000 in Wudinghe basin.

29

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

482

483 484

Figure. 3. Location of Tongtianhe basin.

30

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

485

486 487

Figure. 4. Mean monthly precipitation and runoff from 1980 to 2013 in Tongtianhe basin.

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488

489 490 491

Figure. 5. Model parameters (evapotranspiration parameter C, water storage capacity SC) of assimilated and true in the synthetic experiment, considering C and SC are periodicity and increasing trend, respectively.

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492

493 494 495

Figure. 6. Model parameters (evapotranspiration parameter C, water storage capacity SC) of assimilated and true in the synthetic experiment, considering C and SC are periodicity and abrupt change, respectively.

33

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496

497 498 499 500

Figure. 7. Model parameters (evapotranspiration parameter C, water storage capacity SC) of assimilated and true in the synthetic experiment, considering C is periodicity with an increasing trend and SC is increasing trend, respectively.

34

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501

502 503 504

Figure. 8. Model parameters (evapotranspiration parameter C, water storage capacity SC) of assimilated and true in the synthetic experiment, considering C is periodicity with an increasing trend and SC is abrupt change, respectively.

35

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505

506 507 508

Figure. 9. Double mass curve of monthly runoff and precipitation for Wudinghe basin within the period 1958-2000 (top figure) and Tongtianhe basin within the period 1982-2013 (bottom), respectively.

36

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509

510 511 512 513

Figure. 10. Estimated parameter values of SC (water storage capacity) and associated 95% uncertainty intervals for Wudinghe basin within the period 1958-2000 (top figure) and Tongtianhe basin within the period 1982-2013 (bottom).

37

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514

515 516 517 518

Figure. 11. Estimated parameter values of C (evapotranspiration parameter) and associated 95% uncertainty intervals for Wudinghe basin within the period 1958-2000 (top figure) and Tongtianhe basin within the period 1982-2013 (bottom).

38

Hydrol. Earth Syst. Sci. Discuss., doi:10.5194/hess-2015-407, 2016 Manuscript under review for journal Hydrol. Earth Syst. Sci. Published: 26 January 2016 c Author(s) 2016. CC-BY 3.0 License.

519

520 521 522

Figure. 12. Comparison of observed runoff and runoff estimations from the EnKF and SCE-UA for Wudinghe basin within the period 1958-2000 (top figure) and Tongtianhe basin within the period 1982-2013 (bottom).

39